ABSTRACTWe calculate double‐resonance Raman (DRR) spectra of monolayer graphene by first‐principles density functional calculation, for wide laser excitation energies from the near‐infrared (1.58 eV) to the deep‐ultraviolet (DUV, 5.41 eV) region. When laser excitation energy, , goes into the DUV region, Raman peak wavenumber for G band switches from red‐shift to blue‐shift and for 2D band switches from red‐shift to constant, in contrast to the continuous blue‐shift of G band. Raman intensity of the three bands generally decreases with increasing , except for around 4.08 eV where Raman intensity diverges due to van Hove singularity of electron density of states. The combined two‐phonon modes change with for both G and G bands (e.g., from 2LO to 2TO and back to 2LO for G and from LA + LO/TO to TA + LO/TO for G) but remain 2LO for 2D band. Further, the dominant DRR scattering process of G band changes from the electron‐hole ( or ) scattering processes to the scattering processes as goes into the DUV region, since the Dirac energy bands become asymmetric between and band that suppresses the process and the Raman intensity. Another factor to suppress the Raman intensity is the quantum interference effect between four scattering processes () which changes from constructive to destructive interference and finally to no interference with increasing . We calculate ‐dependent Raman tensor of the three bands and polarized Raman spectra, which further support the interference effect. The calculated results are directly compared and consistent with the experimental results.
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